Transcript An oscilloscope consists of a specially made electron tube and

Thermionic emission
• If a tungsten filament is heated to about
2000 o C, some of the electrons have
sufficient kinetic energy to escape from the
surface of the wire.
• This effect is called thermionic emission.
• It is quite easy to imagine this if we think
about a metal wire as a lattice of ions in a
sea of free electrons. In effect we are
boiling the electrons off.
Thermionic Diode
• In the vacuum tube there are
two electrodes
• Cathode -ve
Anode +ve
• When the filament is
switched on electrons start
to flow from the cathode the
tungsten filament and are
attracted to the anode
• You need a vacuum as the
electrons would collide with
the gas particles. Also the
filament would burn up
Deflection tube
• The electron gun
consists of a heated
filament/cathode and an
anode with a hole in it.
• This produces a narrow
beam of electrons
• The screen is coated
with a fluorescent
material which glow
when electrons strike it.
Deflection Tube
Defection by an electric field
• The negatively charged electrons are
attracted towards the positive plate.
Deflection tube
• In a magnetic field the electron is deflected
depending on the direction of the magnetic
field - Use Lenz’s left hand rule.
Cathode Ray Tubes
Thermionic emission was the starting point
for Joseph John Thomson to produce his
cathode ray tube (CRT) in 1897, the
descendants of which we used to see every
day, before TFT (thin film transistor) TV sets
became more common.
• Now do question 1 page 243
Using an Oscilloscope
Learning Objectives

To know what an oscilloscope is and how it
works.

To know how to measure the pd of alternating
current and direct current.

To know how to measure the frequency of an
alternating current.
Cathode Ray Oscilloscope
Definition

From the specification book:-

An oscilloscope consists of a specially made
electron tube and associated control circuits.

The electron gun emits electrons towards a
fluorescent screen  light is emitted when
electrons hit the screen  this is what we see.
Tube Photograph
Electron Gun Photograph
Tube Diagram
y plates - amplifier
anode
x plates - timebase
heater
supply
- +
H.T. supply
fluorescent
screen
Cathode Ray Oscilloscope
(CRO)
Time base
Display
Y-gain
My tie
Channel1
Channel 2
How does it work?

An oscilloscope consists of a specially made
electron tube and associated control circuits.

An electron gun at one end of the glass tube
emits electrons in a beam towards a fluorescent
screen at the other end of the tube.

Light is emitted from the spot on the screen
where the beam hits the screen.
How does it work?

When no p.d. is applied across the plates the
spot on the screen is stationary.

If a pd is applied across the X-plates the beam
of electrons is deflected horizontally and the
spot moves across.

pd across Y-plates  spot moves up and down.
Reading the CRO 1
Peak-toPeak
voltage
Time Period (ms)
To get the time period you
need to measure this distance
and convert it to time by
multiplying by the time base
setting
Oscilloscope Controls

The x-plates are connected to a time base circuit
which is designed to make the spot move across
the screen in a given time  then back again
much faster.  a bit like a trace on a heart
monitor.

The y-plates are connected to the Y-input and
this causes the spot to move up or down
depending on the input pd.
electron gun
produces a beam
of electrons
summary
y plates
anode
heater
supply
light produced on
the screen by
electron beam
x plates
a p.d. across the y
- + deflects the
plates
vertically
H.T. trace
supply
a p.d. across the x
plates deflects the
phosphor
trace
horizontally
screen
Oscilloscope Controls

The gain sets the scale for the y-axis, normally in
volts per cm.

The time base sets the scale for the x-axis,
normally in ms per cm.

Recall that frequency can be calculated from the
period from the graph using:
1
frequency 
period
Displaying a waveform
1. The time base
• The X-plates are connected to the
oscilloscope’s time base circuit.
• This makes the spot move across
the screen, from left to right, at a
constant speed.
• Once the spot reaches the right
hand side of the screen it is
returned to the left hand side
almost instantaneously.
• The X-scale opposite is set so that
the spot takes two milliseconds to
move one centimetre to the right.
(2 ms cm-1).
NTNU Oscilloscope Simulation
KT Oscilloscope Simulation
Gain and Time-Base Controls
Displaying a waveform
2. Y-sensitivity or Y-gain
• The Y-plates are connected to
the oscilloscope’s Y-input.
• This input is usually amplified
and when connected to the Yplates it makes the spot move
vertically up and down the
screen.
• The Y-sensitivity opposite is set
so that the spot moves
vertically by one centimetre for
a pd of five volts (5 V cm-1).
• The trace shown appears when
an alternating pd of 16V peakto-peak and period 7.2 ms is
connected to the Y-input with
the settings as shown.
NTNU Oscilloscope Simulation
KT Oscilloscope Simulation
Peak Voltage
Peak p.d. = 3 Divisions x 1.0 mV/div = 3.0 mV
Period & Frequency
period = 4.0 divisions x 1.0 ms/div = 4.0 ms
frequency = 1 / period
frequency = 1 / 0.004 s
frequency = 250 Hz
Measuring d.c. potential difference
All three diagrams below show the trace with the time base
on and the Y-gain set at 2V cm-1.
Diagram a shows the trace for pd = 0V.
Diagram b shows the trace for pd = +4V
Diagram c shows the trace for pd = -3V.
NTNU Oscilloscope Simulation
KT Oscilloscope Simulation
Measuring a.c. potential difference
Let the time base setting be 10ms cm-1 and the
Y-gain setting 2V cm-1.
In this case the waveform performs one
complete oscillation over a horizontal distance
of 2 cm.
Therefore the period of the waveform
is 2 x 10ms
period = 20 ms
as frequency = 1 / period
frequency = 1 / 0.020s
= 50 Hz.
NTNU Oscilloscope Simulation
KT Oscilloscope Simulation
The peak-to-peak displacement of the waveform
is about 5cm.
Therefore the peak-to-peak pd is 5 x 2V
Peak-to-peak pd = 10V
Self Test
The oscilloscope ‘graph’ scales
Y-AXIS
Potential
difference
+V
Scale determined
by the ‘Y-GAIN’
control
0V
Typical setting:
1V / cm
-V
cm squares
X-AXIS
Time
Scale determined by the ‘X-GAIN’ or ‘TIME-BASE’ control
Typical setting: 0.1s / cm
Question 1
Measure the approximate
period, frequency and peakto-peak pd of the trace
opposite if:
Time base = 5ms cm-1
Y-gain = 5V cm-1
period = 50ms / 6 ≈ 8.7ms
frequency ≈ 115 Hz
peak-to-peak pd ≈ 20V
Question 2
Measure the approximate
period, frequency and peak
pd of the trace opposite if:
Time base = 2ms cm-1
Y-gain = 0.5V cm-1
period = 20ms / 12 ≈ 1.7ms
frequency ≈ 600 Hz
peak pd ≈ 1.3V
Question 3
The trace shows how a waveform of
frequency 286 Hz and peak-to-peak pd
6.4V is displayed.
Suggest the settings of the time base and
Y-gain amplifier.
The period of a wave of frequency 286Hz
= 1/285 = 0.0035s = 3.5ms
One complete oscillation of the trace
occupies 7cm.
Therefore time base setting is 3.5ms / 7cm
≈ 0.5 ms cm-1
The peak-to-peak displacement of the
trace is about 3.7 cm.
Therefore the Y-gain setting is 6.4V /
3.7cm
≈ 2V cm-1
Application

Measuring the speed of ultrasound.

Set up the oscilloscope so that the time base
circuit triggers a transmitter to send out a pulse
of ultrasonic waves.

The receiver can be connected to the Y-input of
the oscilloscope so that the waveform can be
seen on the screen when it is detected.
Internet Links
• Oscilloscope - basic display function NTNU
• Oscilloscope Simulation - by KT
• Lissajous figures - Explore Science
• Lissajous figures - by KT